tunable topological phononic crystals - hkust …ias.ust.hk/events/201601wp/doc/presentation...
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Tunable topological phononic crystals
Zeguo Chen (陈泽国) and Ying Wu (吴莹) King Abdullah University of Science and Technology
12 Jan 2016, Hong Kong
Outline
• Introduction – Background and motivation
• Tunable topological phononic crystals – Design – Physical model – Topological properties – Demonstration
• Summary
Introduction
Nat. Phys. 11, 799 (2015) Rev. Mod. Phys. 82 3045 (2010)
One way propagaFon edge states.
• QH state
• QSH states
TKNN invariant
• Chern number. – Arises from topology that differentiates QH (non-trivial)
and an ordinary insulator (trivial). – Integration of Berry flux in the BZ.
Cm =12π
d 2∫k∇×
Am
Am = i um ∇k umBerry connecFon
Nat. Photonics 8 821 (2014)
Classical analogues in photonic systems
Phys. Rev. LeK. 100, 013905 (2008) Phys. Rev. LeK. 100, 013904 (2008).
YIG material
About acoustics
• Breaking Time-reversal symmetry in acoustics
Nonreciprocal air-flow-contained acoustic circulator
Science 343, 516 (2014)
Motivation
• From deterministic degeneracy at K point to accidental degeneracy at point Γ
Protected by TRS
Accidental degeneracy
What happens if Fme-‐reversal symmetry is broken and ,at the same Fme, geometry changes as well?
PRB 86 035141 (2012)
Sample
0r1r d
0 0.35r m=
1 0.5r m=
2a m=
−ρc2iω(iωφ + v ⋅∇φ)+∇⋅ (ρ∇φ − ρ
c2(iωφ + v ⋅∇φ)v) = 0
v = 0No air flow
22 ( ) 0cρω φ ρ φ+∇⋅ ∇ =
100
120
140
160
180
200
ΜΧΓΜ
Frequency(Hz)
0 0.07336d m=
0.04 0.06 0.08 0.10125
130
135
140
145
150
ϕpx, ϕpy ϕd
Freq
uenc
y(H
z)
d(m)
d1 d0 d2
Gap 11 12 12
12 22 22
12 22 22
2 (cos cos ) 2 sin 2 sin2 sin 2 cos 2 cos 02 sin 0 2 cos 2 cos
d x x y x x x y
x x px x x y y
x y py y x x y
E t k a k a it k a it k aH it k a E t k a t k a
it k a E t k a t k a
⎡ ⎤+ +⎢ ⎥= − + +⎢ ⎥⎢ ⎥− + +⎣ ⎦
tmij = Φi (
r ) H Φ j (r + rm )
A tight-binding model
k = 0
11
22 22
22 22
2 0 00 2 2 00 0 2 2
d x
px x y
py y x
E tH E t t
E t t
⎡ ⎤+⎢ ⎥= + +⎢ ⎥⎢ ⎥+ +⎣ ⎦
mainly contributed by the wave funcFons inside the waveguide
E is the on-‐site energy of the rings
Eigenvalue depends on the width of the waveguide.
Breaking T Symmetry: with air flow
0 5 10 15130
132
134
136
138
140
142
Freq
uenc
y(H
z)
v (m/s)
ϕd
ϕpx
ϕpyv(x, y) = ( −vy
x2 + y2, vx
x2 + y2) = veθ
( ) avc v Rω± = ± ( )0 1 2avR r r= +
From C4v to C4. almost does not change ϕd
Degeneracy is li`ed.
d = d0
Band structures
Χ ΜΓΜΧΓ
100
120
140
160
180
200
Frequency(Hz)
ΧΓ ΜΜ
• Degeneracy associated with and li`s.
• Branch associated with almost does not change.
Consistent with the Tight-‐Binding.
pxϕ pyϕ
dϕ
0.04 0.06 0.08 0.10125
130
135
140
145
150
Freq
uenc
y(H
z)
d(m)
ϕpx
ϕpy
ϕd
d1dt d2
0.04 0.06 0.08 0.10125
130
135
140
145
150
ϕpx, ϕpy ϕd
Freq
uenc
y(H
z)
d(m)
d1 d0 d2
Topological property: Chern number
C = i2π
∇ k × un (k )
BZ∫n∑ ∇ k un (
k ) d 2
k
( ) ( ) (Y)Cj j j
j
i ξ ξ ζ= Γ Μ∏
Phys. Rev. B 86, 115112 (2012)
0.04 0.06 0.08 0.10125
130
135
140
145
150
Freq
uenc
y(H
z)
d(m)
ϕpx
ϕpy
ϕd
d1dt d2
100
120
140
160
180
200
Frequency(Hz)
0
ΧΓ ΜΜ
0
Trivial
100
120
140
160
180
200
ΜΧΓΜ
Frequency(Hz)
1
0
Non-‐trivial
100
120
140
160
180
200
2
-1
ΧΜ Μ
Frequency(Hz)
Γ
Trivial Non-‐trivial
TransiFon point
TransiFon point depends on: geometry & intensity of the flow
Tunable!
Topological properties
C=0 C=1 C=1
Demonstration II: fixed geometry
Trivial
Non-‐trivial
0 5 10 15137
138
139
Freq
uenc
y(H
z)
v (m/s)
ϕd
ϕpy
0.065d m=
Summary
• Designed a topological phononic crystal • Topological property depends on both the
geometry and time-reversal symmetry • One-way propagation edge state is
observed. • Tunable property is demonstrated.
Acknowledgement: • KAUST baseline research fund.
Thank you. More informaFon: hKp://arxiv.org/abs/1512.00814 [email protected] [email protected]